Chapter 14: Problem 2061
Alternating current cannot be measured by dc ammeter because, (a) ac cannot pass through dc ammeter (b) Average value of complete cycle is zero (c) ac is virtual (d) ac changes its direction
Chapter 14: Problem 2061
Alternating current cannot be measured by dc ammeter because, (a) ac cannot pass through dc ammeter (b) Average value of complete cycle is zero (c) ac is virtual (d) ac changes its direction
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Get started for freeIn an ac circuit, the current is given by $\mathrm{I}=5 \sin [100 \mathrm{t}-(\pi / 2)]\( and the ac potential is \)\mathrm{V}=200 \sin 100 \mathrm{t}$. Then the power consumption is, (a) 20 watts (b) 40 watts (c) 1000 watts (d) 0 watts
A wire of length \(2 \mathrm{~m}\) is moving at a speed \(2 \mathrm{~ms}^{-1}\) keep its length perpendicular to uniform magnetic field of \(0.5 \mathrm{~T}\). The resistance of circuit joined with this wire is \(6 \Omega\). The rate at which work is being done to keep the wire moving at constant speed is ........... (a) \((1 / 3) \infty\) (b) \((2 / 3) \omega\) (c) \((1 / 6) \propto\) (d) \(2 \mathrm{c}\)
A coil having n turns \(\&\) resistance \(R \Omega\) is connected with a galvanometer of resistance \(4 \mathrm{R} \Omega\). This combination is moved from a magnetic field \(\mathrm{W}_{1} \mathrm{~Wb}\) to $\mathrm{W}_{2} \mathrm{~Wb}\( in \)\mathrm{t}$ second. The induced current in the circuit is.... (a) $-\left[\left\\{\mathrm{W}_{2}-\mathrm{W}_{1}\right\\} /\\{5 \mathrm{Rnt}\\}\right]$ (b) $-\mathrm{n}\left[\left\\{\mathrm{W}_{2}-\mathrm{W}_{1}\right\\} /\\{5 \mathrm{Rt}\\}\right]$ (c) $-\left[\left\\{\mathrm{W}_{2}-\mathrm{W}_{1}\right\\} /\\{\mathrm{Rnt}\\}\right]$ (d) $-\mathrm{n}\left[\left\\{\mathrm{W}_{2}-\mathrm{W}_{1}\right\\} /\\{\mathrm{Rt}\\}\right]$
A 20 volts ac is applied to a circuit consisting of a resistance and a coil with negligible resistance. If the voltage across the resistance is $12 \mathrm{~V}$, the voltage across the coil is, (a) 16 volts (b) 10 volts (c) 8 volts (d) 6 volts
The quality factor of LCR circuit having resistance \((\mathrm{R})\) and inductance ( \(\mathrm{L}\) ) at resonance frequency \((\infty)\) is given by (a) \((\mathrm{cL} / \mathrm{R})\) (b) \((\mathrm{R} / \mathrm{cL})\) (c) \((\mathrm{coL} / \mathrm{R})^{(1 / 2)}\) (d) \((0 / L)^{2}\)
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